4W
To solve this problem, we need to analyze the energy dissipation rate before and after the wire is cut.
Initial Energy Dissipation Rate: The power P dissipated by a resistor is given by:
\( P = \frac{V^2}{R} \),
where: - V is the voltage across the resistor, and R is the resistance.
Initially, with resistance R, the energy dissipation rate is:
\( W = P = \frac{V^2}{R} \).
After Cutting the Wire: When the wire is cut into two halves, each half has a resistance of:
\( R' = \frac{R}{2} \).
Connecting in Parallel: When these two halves are connected in parallel, the equivalent resistance Req is given by:
\( \frac{1}{R_{eq}} = \frac{1}{R'} + \frac{1}{R'} = \frac{2}{R/2} = \frac{4}{R} \).
Thus, the equivalent resistance is:
\( R_{eq} = \frac{R}{4} \).
New Energy Dissipation Rate: The new power P' dissipated in the circuit with the new resistance Req is:
\( P' = \frac{V^2}{R_{eq}} = \frac{V^2}{R/4} = \frac{4V^2}{R} \).
Comparing Power Dissipation Rates: Since \( W = \frac{V^2}{R} \) from the original circuit, we can relate the new power:
\( P' = 4W \).
The problem describes a scenario where a wire dissipates energy at a rate \(W\) when connected to a potential difference \(V\). We need to determine the new rate of energy dissipation when the wire is cut into two equal halves and these halves are connected in parallel to the same voltage supply.
The solution relies on the fundamental principles of electrical resistance and power dissipation.
Step 1: Define the initial state.
In the initial setup, the full wire has a resistance \(R\). When a potential difference \(V\) is applied across it, the energy dissipation rate is \(W\).
Using the power formula, we can write:
\[ W = \frac{V^2}{R} \]
This equation serves as our reference for the initial power dissipation.
Step 2: Determine the resistance of the cut pieces.
The wire is cut into two equal halves. Since resistance is directly proportional to length, the resistance of each half (\(R_{\text{half}}\)) will be half of the original resistance \(R\).
\[ R_{\text{half}} = \frac{R}{2} \]
Step 3: Calculate the equivalent resistance of the parallel combination.
These two halves, each with resistance \(R_{\text{half}} = R/2\), are connected in parallel. Let the new equivalent resistance be \(R_{\text{parallel}}\).
\[ \frac{1}{R_{\text{parallel}}} = \frac{1}{R_{\text{half}}} + \frac{1}{R_{\text{half}}} = \frac{1}{R/2} + \frac{1}{R/2} \] \[ \frac{1}{R_{\text{parallel}}} = \frac{2}{R} + \frac{2}{R} = \frac{4}{R} \]
Solving for \(R_{\text{parallel}}\), we get:
\[ R_{\text{parallel}} = \frac{R}{4} \]
Step 4: Calculate the new energy dissipation rate.
The parallel combination is connected across the same voltage supply \(V\). Let the new energy dissipation rate be \(W_{\text{new}}\).
Using the power formula with the new equivalent resistance:
\[ W_{\text{new}} = \frac{V^2}{R_{\text{parallel}}} \]
Substitute the value of \(R_{\text{parallel}} = R/4\) into this equation:
\[ W_{\text{new}} = \frac{V^2}{(R/4)} \]
Simplifying the expression for the new power dissipation:
\[ W_{\text{new}} = 4 \left( \frac{V^2}{R} \right) \]
From Step 1, we know that the original power dissipation is \(W = \frac{V^2}{R}\). Substituting this into our expression for \(W_{\text{new}}\):
\[ W_{\text{new}} = 4W \]
Therefore, the energy dissipation rate will become 4W.

The following are the graphs of potential barrier versus width of the depletion region for a p-n junction diode. 
Which of the following is correct?


The integral is given by:
\[ 80 \int_{0}^{\frac{\pi}{4}} \frac{\sin\theta + \cos\theta}{9 + 16 \sin 2\theta} d\theta \]
is equals to?
A P-N junction is an interface or a boundary between two semiconductor material types, namely the p-type and the n-type, inside a semiconductor.
in p-n junction diode two operating regions are there:
There are three biasing conditions for p-n junction diode are as follows: